A Comparison of Allylic and Propargylic Radicals - American

state energies than radical or transition-state properties. No study ... bp 95" (17 mm)]; / i Z 0 ~. 1.4353 (lit.12 ~z*OD ... flask containing 19.6 g ...
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3771 6.08 (l,l,l-trichloroheptene-2)and 6.17 p (1,1,3-trichloroheptene-1). The nmr spectrum showed a complicated pattern of absorption in the T 3.6-4.7 region, which was shown to result from a 12-line ABX2 system (l,l,l-trichloroheptene-2)and a doublet (1,1,34richloroheptene-1). The isomerization of l,l,l-trichloroheptene-2 to its allylic isomer was easily followed by means of the nmr spectrum: l,l,l-trichloroheptene-2:T A 3.73, T B 4.40, JAB = 11.46 cps, JAX?= 1.92 cps; 1,1,3-trichloroheptene-2: T A 4.0, T B 5.4, J A B = 9.7 cps. Isomerization was accomplished by heating a sealed nmr tube containing the product in an oven maintained at 95" for 6 hr or more. The addition of thionyl chloride to the product catalyzed isomerization at room temperature.

The Addition of Bromotrichloromethane to Heptyne-1. Heptyne-1 (0.1 mole) and BrCC18 (0.4 mole) were transferred into a quartz tube, flushed with nitrogen, and sealed under vacuum. The tube was irradiated for 6 hr with ultraviolet light from a 200-w Hanovia lamp. The reaction mixture was distilled to yield one major product, bp 72-74" (0.02 mm). The infrared and nmr spectra of the distillate indicated that it was the heptyne-1-BrCCla 1 :1 normal adduct. The infrared spectrum showed bands at 6.17 (C=C) and 7.22 p (gem-dimethyl); nmr: triplet at T 3.2 (J = 0.8 cps, 1.0 H), multiplet at T 7.2 (2.0 H), and doublet at T 9.1 (J = 6 cps, 6.0 H). The addition product obtained from the addition of BrCCh to 6-methylheptyne-1,bp 72-74" (0.02 mm), was also found to be the normal 1 :1 adduct.

A Comparison of Allylic and Propargylic Radicals Michael M. Martin' and Edward B. Sanders2 Contributionf r o m the Department of Chemistry, University of Michigan, Ann Arbor, Michigan. Received March 15,1967 Abstract: Through a study of the thermal, homolytic concerted decompositions of the B,y-olefinic and P,y-acetylenic peresters Ia-f, activation parameters for processes generating allylic and propargylic radicals have been determined. These activation parameters establish that the 2-buten-1-yl radical (Ira) is about 4 kcalimole more stable than the 2-butyn-1-yl radical (IIb), but that the additional stability of the allylic radical is achieved only through the imposition of rotational restrictions not imposed upon the propargyl radical. Radical stabilization through delocalization in a propargyl radical requires no rotational restrictions as a consequence of the cylindrical symmetry of the triple bond. The y-phenyl group of the 3-phenyl-2-propen-1-yl radical (IId) increases the stability of the radical by extending the conjugated system, whereas the y-phenyl group of the 3-phenyl-2-propyn-1-yl radical (IIe) confers very little added stability to the propargyl radical, suggesting that the delocalization of the free electron does not extend into the benzene ring.

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he formation of allylic free radicals through hydrogen abstraction is the first step in a number of synthetically useful reactions, such as allylic halogenation with N-bromos~ccinimide~ and t-butyl hypochlorite.4 Analogous reactions, utilizing acetylenic substrates,5!6 though less frequently employed, also reflect the possibility of selective hydrogen abstraction at a propargylic position. The origin of the greater ease of abstraction

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I \ of an allylic or propargylic atom when compared t o hydrogen abstraction from carbon atoms not adjacent to multiple bonds is obviously the formation of resonance-stabilized radicals, the contributing canonical forms for which are depicted in eq 1 and 2. It is important t o recognize, however, that there are some significant differences between allylic and propargylic radicals and consequently also between processes which generate them. For instance, the two contribu t i n g canonical forms of the allylic radical are struc(1) Alfred P. Sloan Foundation Fellow. (2) Petroleum Research Fund Predoctoral Fellow, 1964-1966. (3) W. Pryor, "Free Radicals," McGraw-Hill Book Co., Inc., New York, N. Y . , 1966, pp 195-197. (4) C. Walling and W. Thaler, J . Am. Chem. SOC.,83, 3877 (1961). ( 5 ) A. Wohl and K. Jaschinowski, Ber., 54, 476 (1921). (6) C. Walling, L. Heaton, and D. Tanner, J . Am. Chem. SOC.,87, 1715(1965).

turally similar and therefore of very similar energies, whereas the two contributing structures of the propargyl radical, one acetylenic and one allenic, are not of equal energies. Hence, it would be anticipated that resonance stabilization of an allylic radical would be greater than for a propargylic radical. Bond energy data tend to support this contention. Although there is rather wide variation in bond disssociation values reported for allylic and propargylic bonds when measured by different methods, allylic bond dissociation energies are generally about 3-4 kcal/mole less than propargylic bond dissociation energies when measured by the same method in analogous comp~unds.~-~O However, since the formation of a resonance-stabilized allylic radical requires overlap of the three p orbitals involved in the delocalized three-electron system, rotation of the bond between the allylic carbon atom and the double bond is necessarily restricted in the radical. There are no such restrictions in the propargyl radical, since the cylindrical symmetry of a triple bond permits overlap of the p orbital on the propargylic carbon atom in any rotational state. Thus an allyl radical is more stable than a n analogous propargyl radical, but its added stability is purchased at the price of a loss in rotational freedom. Hence, one would be led to expect that a process leading to an allylic radical would have a lower enthalpy of (7) M. Szwarc, J . Chem. P h j s . , 17, 284, 292 (1949). (8) C. A. McDowell, F. P. Lossing, I. H. S. Henderson, and J. P. Farmer, Can. J . Chem., 34, 345 (1956). (9) K. W. Egger, D. M. Golden, and S. W . Benson, J . Am. Chem. Soc., 86, 5420 (1964). (10) J. Collin and F. P. Lossing, ibid., 79, 5848 (1957).

Martin, Sanders / Allylic and Propargylic Radical Comparison

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activation and a more negative entropy of activation than one leading to a structurally analogous propargyl radical. It is not apparent, a priori, how these two opposing factors will balance out. Gazith and Szwarc'l have found that a methyl radical abstracts a hydrogen atom from a position adjacent to a triple bond about twice as readily as from a position adjacent t o a double bond, whereas Walling, Heaton, and Tanner6 have found that a t-butoxy radical abstracts allylic hydrogen atoms about 1.5 times as readily as propargylic hydrogen atoms. Both of these studies involve rather exothermic reactions and more likely reflect differences in groundstate energies than radical or transition-state properties. No study designed t o establish the relative abilities of a double and triple bond t o facilitate radical formation at adjacent positions has appeared. In this paper a series of studies is reported in which structurally analogous allylic and propargylic radicals are generated endothermally by concerted perester decompositions (reaction 3). By a kinetic study of the p-cymene

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